System and method for routing signals in complex quantum systems

ABSTRACT

Embodiments of the present invention disclose a computer system having a plurality of quantum circuits arranged in a two-dimensional plane-like structure, the quantum circuits comprising qubits and busses (i.e., qubit-qubit interconnects), and a method of formation therefor. A quantum computer system comprises a plurality of quantum circuits arranged in a two-dimensional pattern. At least one interior quantum circuit, not along the perimeter of the two-dimensional plane of the plurality of quantum circuits, contains a bottom chip, a device layer, a top chip, and a routing layer. A signal wire connects the device layer to the routing layer, wherein the signal wire breaks the two dimensional plane, for example, the signal wire extends into a different plane.

BACKGROUND

The present invention relates generally to the field of quantumcomputing systems, and more particularly to wiring for interior quantumcomputing circuits.

BRIEF SUMMARY

Additional aspects and/or advantages will be set forth in part in thedescription which follows and, in part, will be apparent from thedescription, or may be learned by practice of the invention.

Embodiments of the present invention disclose a computer system having aplurality of quantum circuits arranged in a two-dimensional plane-likestructure, the quantum circuits comprising qubits and busses (i.e.,qubit-qubit interconnects), and a method of formation therefor. Aquantum computer system comprises a plurality of quantum circuitsarranged in a two-dimensional pattern. At least one interior quantumcircuit, meaning a quantum circuit not along the perimeter of thetwo-dimensional plane of the plurality of quantum circuits, contains abottom chip, a device layer, a top chip, and a routing layer. A signalwire connects the device layer to the routing layer, wherein the signalwire breaks (i.e., is not parallel to) the two dimensional plane, forexample, the signal wire extends into a different plane.

BRIEF DESCRIPTION OF THE DRAWINGS

The above and other aspects, features, and advantages of certainexemplary embodiments of the present invention will be more apparentfrom the following description taken in conjunction with theaccompanying drawings, in which:

FIG. 1 is an interior quantum circuit, not along the perimeter of thetwo-dimensional plane of the plurality of quantum circuits, inaccordance with an embodiment of the present invention;

FIG. 2 is an exploded view of the quantum circuit, in accordance with anembodiment of the present invention;

FIGS. 3A-3C illustrates a wire bonding process to the quantum circuit,in accordance with an embodiment of the present invention; and

FIG. 4 illustrates a method of the wire bonding process to the quantumcircuit, in accordance with an embodiment of the present invention.

DETAILED DESCRIPTION

The following description with reference to the accompanying drawings isprovided to assist in a comprehensive understanding of exemplaryembodiments of the invention as defined by the claims and theirequivalents. It includes various specific details to assist in thatunderstanding but these are to be regarded as merely exemplary.Accordingly, those of ordinary skill in the art will recognize thatvarious changes and modifications of the embodiments described hereincan be made without departing from the scope and spirit of theinvention. In addition, descriptions of well-known functions andconstructions may be omitted for clarity and conciseness.

The terms and words used in the following description and claims are notlimited to the bibliographical meanings, but, are merely used to enablea clear and consistent understanding of the invention. Accordingly, itshould be apparent to those skilled in the art that the followingdescription of exemplary embodiments of the present invention isprovided for illustration purpose only and not for the purpose oflimiting the invention as defined by the appended claims and theirequivalents.

It is to be understood that the singular forms “a,” “an,” and “the”include plural referents unless the context clearly dictates otherwise.Thus, for example, reference to “a component surface” includes referenceto one or more of such surfaces unless the context clearly dictatesotherwise.

For purposes of the description hereinafter, terms such as “upper”,“lower”, “right”, “left”, “vertical”, “horizontal”, “top”, “bottom”, andderivatives thereof shall relate to the disclosed structures andmethods, as oriented in the drawing figures. Terms such as “above”,“overlying”, “atop”, “on top”, “positioned on” or “positioned atop” meanthat a first element, such as a first structure, is present on a secondelement, such as a second structure, wherein intervening elements, suchas an interface structure may be present between the first element andthe second element. The term “direct contact” means that a firstelement, such as a first structure, and a second element, such as asecond structure, are connected without any intermediary conducting,insulating or semiconductor layers at the interface of the two elements.

In the interest of not obscuring the presentation of embodiments of thepresent invention, in the following detailed description, someprocessing steps or operations that are known in the art may have beencombined together for presentation and for illustration purposes and insome instances may have not been described in detail. In otherinstances, some processing steps or operations that are known in the artmay not be described at all. It should be understood that the followingdescription is rather focused on the distinctive features or elements ofvarious embodiments of the present invention.

Reference will now be made in detail to the embodiments of the presentinvention, examples of which are illustrated in the accompanyingdrawings, wherein like reference numerals refer to like elementsthroughout. Embodiments of the invention are generally directed to aninterior quantum circuit in a quantum system.

In embodiments of the present invention, a quantum system contains atwo-dimensional (2D) lattice of qubits connected by busses. Embodimentsof the present invention provide structures, and fabrication methodstherefor, for input/output wiring for the quantum circuits arranged inthe interior of the lattice. A top-chip (routing chip) may be mounted ontop of a bottom chip (device chip), and made from highly purecrystalline silicon. The routing chip may have a routing layer withtransmission lines patterned on it without the risk of disturbing qubitsin the device chip. The device chip may include a device layer with aplurality of qubits connected by busses. In order to route signals fromthe routing layer to the device layer, embodiments of the presentinvention disclose fabricating “through holes” in the top chip. Thesignal is then transported from a routing layer of the top-chip to thedevice layer of the bottom chip through a wirebond. In some embodiments,the wirebond is placed though the through hole using a ball-bondingtool, which may allow very narrow capillaries (placing the wire) to beused. Reducing the size of the through hole used allows for more compactcircuits. For the top-chip, a standard 8 inch silicon wafer can be used(thicknesses on the order of 750 microns) and through holes can have adiameter of 100 μm to 1000 μm. The diameter of the through hole islimited by the amount of available space. In one embodiment, the throughhole has a diameter of 500 μm. Connecting the interior quantum circuitsusing a through hole allows for the signal lines to be routed to thequbits located on the interior of the lattice and enables communicationof the interior qubits with structures outside the two dimensionalplane.

FIG. 1 is an interior quantum circuit, not along the perimeter of thetwo-dimensional plane of the plurality of quantum circuits, inaccordance with an embodiment of the present invention. FIG. 2 is anexploded view of the quantum circuit, in accordance with an embodimentof the present invention.

The interior quantum circuit 100 includes a bottom chip 105, a devicelayer 107, a top chip 109, a routing layer 111, signal lines 113,bonding pads 115, bond wires 117, and through holes 119. The explodedview of the interior quantum circuit 100, as illustrated by FIG. 2,further illustrates a quantum bit 121, a readout resonator 123, and abond pad of bonding pads 127. Only one bonding pad of bonding pads 127is depicted in FIG. 2, but it should be understood that device layer 107includes a second bond pad (not shown) that is obscured by a portion oftop chip 109. Each of bonding pads 127 is located below and aligned witha through hole of though holes 119.

The device layer 107 is formed on top of the bottom chip 105. The devicelayer 107 includes structures that may comprise at least onesuperconducting material, for example, Niobium, Aluminum, or othersuitable materials. In the depicted embodiment, device layer 107includes the readout resonator 123, the quantum bit 121, and the bondpad 127.

The quantum bit 121 is a structure that processes units of quantuminformation (called qubits) that are the quantum analogue of theclassical bit. A qubit is a two-state quantum-mechanical system, such asthe polarization of a single photon: here the two states are verticalpolarization and horizontal polarization. In a classical system, a bitwould have to be in one state or the other. However, quantum mechanicsallows the qubit to be in a superposition of both states at the sametime, a property that is fundamental to quantum computing.

In example embodiments of the present invention, the qubit includes thefollowing properties: during measurement, the qubit is projected intoone of two different states (IA> or IB>). A successful read-out occurswhile the two states IA> and IB> are stable, after which the qubit maydecohere. The readout resonator attains a resonance frequency based uponthe state of the projected qubit.

The projected state of the qubit can be inferred based on the readoutresonator frequency, which can be determined based on the reflection ortransmission coefficient of the readout resonator. This can beaccomplished through various techniques. In an example technique, amicrowave signal is applied to the input of the circuit and is tuned toa frequency approximately equal to the resonance frequency of one of thepost measurement quasi-stable states in accordance with one exampleembodiment. When the qubit is projected into the measured state, theapplied microwave signal either transmits to the output or is reflectedby the readout resonator, depending on the coupling of the qubit to thetransmission lines. Therefore, depending on the qubit state, themicrowave signal will acquire a specific magnitude and phase. Thedetermination of the qubit state from this signal can be done in avariety of ways, for example, using IQ mixers, threshold detectors andso forth. Other various methods for measuring frequency or state may beused as well.

The top chip 109 is on top of the device layer 107 and includes therouting layer 111, the signal lines 113, and bonding pads 115.

In some embodiments, counter etched patterns (not shown) are formed in abottom surface of top chip 109. In some embodiments, an additionalthrough hole (not depicted) is formed in the top chip 109 directly abovethe bonding pads 127. The counter etched patterns and additional throughhole (not depicted) could potentially help to reduce any induceddecoherence from the top chip 109 even further. The surface of the topchip 109 that faces the device layer 107 could also be coated with asuperconductor, if a counter etched pattern is etched into the top chip109. The counter etched patterns creates a gap between the readoutresonator 123 and the top chip 109, such that the top chip 109 does notcontact the readout resonator 123, thereby preventing the top chip 109from electrically shorting devices on the device layer 107. Coating thisface with a superconducting material reduces unwanted (electromagnetic)crosstalk between devices.

There are several ways that the top chip 109 can be aligned to thedevice layer 107. For example, etched features in the top chip 109 couldbe aligned to patterned features on the bottom chip 105 by aligning thechips visually. If the features are sufficiently large, visual alignmentis possible without use of a microscope.

At least one through hole 119 or a plurality of through holes 119 can becreated in the top chip 109. The through hole 119 can be created in thetop chip 109 using reactive ion etching, bosch process, laser milling,and/or a mechanical process. The through holes 119 can have a diameterof 100 μm to 1000 μm. The diameter of the through hole is limited by theamount of available space. In one embodiment, the through holes 119 havea diameter of 500 μm. In another example, the through hole 119 can belocated in the device layer 107 and the bottom chip 105. This wouldallow the bond wire 117 to pass through the bottom chip 105 to a bottomrouting layer (not shown) that is located on the bottom of bottom chip105.

In conventional complementary metal-oxide semiconductor (CMOS)technology, connecting interior circuits to an output source may be doneby growing dielectric materials on top of the circuit and implementingthrough plated via-structures. This has not been proven to be possiblefor quantum circuits because the microwave quality of depositeddielectrics is too low and would cause qubit decoherence.

Quantum decoherence is the loss of quantum coherence. In quantummechanics, particles such as electrons behave like waves and aredescribed by a wavefunction. These waves can interfere, leading to thepeculiar behavior of quantum particles. As long as there exists adefinite phase relation between different states, the system is said tobe coherent. This coherence is a fundamental property of quantummechanics, and is necessary for the functioning of quantum computers.However, when a quantum system is not perfectly isolated, but in contactwith its surroundings, the coherence decays with time, a process calledquantum decoherence. As a result of this process, the quantum behavioris lost.

Decoherence can be viewed as the loss of information from a system intothe environment, since every system is loosely coupled with theenergetic state of its surroundings. Viewed in isolation, the system'sdynamics are non-unitary (although the combined system plus environmentevolves in a unitary fashion). Thus the dynamics of the system alone areirreversible. As with any coupling, entanglements are generated betweenthe system and environment. These have the effect of sharing quantuminformation with—or transferring it to—the surroundings.

Decoherence has been used to understand the collapse of the wavefunctionin quantum mechanics. Decoherence does not generate actual wave functioncollapse. It only provides an explanation for the observation of wavefunction collapse, as the quantum nature of the system “leaks” into theenvironment. That is, components of the wavefunction are decoupled froma coherent system, and acquire phases from their immediate surroundings.A total superposition of the global or universal wavefunction stillexists (and remains coherent at the global level), but its ultimate fateremains an interpretational issue. Specifically, decoherence does notattempt to explain the measurement problem. Rather, decoherence providesan explanation for the transition of the system to a mixture of statesthat seem to correspond to those states observers perceive. Moreover,observation indicates that this mixture looks like a proper quantumensemble in a measurement situation, as observing that measurements leadto the “realization” of precisely one state in the “ensemble.”

Decoherence represents a challenge for the practical realization ofquantum computers, since such machines are expected to rely heavily onthe undisturbed evolution of quantum coherences. Simply put, theyrequire that coherent states be preserved and that decoherence ismanaged, in order to actually perform quantum computation.

A bond wire 117 is located in through holes 119 to connect bonding pads115 and 127. One advantage of this approach is that the flexibility ofthe bond wire 117 allows for thermal contractions and expansions of thesystem (e.g., top chip 109, bottom chip 105) as it is cooled tocryogenic temperatures (˜10 mK) where the interior quantum circuit 100is operated. An adhesion layer of gold can be placed on top of thebonding pads 115 and 127 on both the device layer 107 and the routinglayer 111. The bonding pads 115 and 127 do not themselves carry quantuminformation and as such can be subject to some microwave losses as wouldoccur when using a non-superconducting material such as gold.

FIGS. 3A-3C illustrate a wire bonding process to the quantum circuit, inaccordance with an embodiment of the present invention. FIGS. 3A-3Cillustrate a ball bonding sequence for an interior quantum circuit 100of FIG. 1, having a bond wire 117 attached to the interior quantumcircuit 100.

In the first step 320 (FIG. 3A), the capillary tool 310 is aligned overthe through hole 305, (which is, for example, is one of through holes119), and the receiving bond pad 127 on the device layer 107. In thesecond step 340 (FIG. 3B), the capillary tool 310 and bond wire 117 islowered into the through hole 305. The melted solder at the end of thebond wire 117 is attached to the receiver bond pad 127 using compressionforce and an ultrasonic pulse. In the final step 360 (FIG. 3C), thecapillary tool 310 is removed from the through hole 305 and the otherend of the bond wire 117 is attached to a corresponding bond pad 115 onthe routing layer 111 using compression and an ultrasonic pulse.

FIG. 4 illustrates a method of the wire bonding process to the quantumcircuit, in accordance with an embodiment of the present invention.

A through hole 119 is formed through the routing layer 111 and the topchip 109 (S410). The top chip 109 is placed on top of the device layer107 (S415). These steps illustrate that the through hole 119 is formedwhile the top chip 109 is separate from the bottom chip 105, but, inother embodiments, the through hole 119 can be formed when the top chip109 has already be aligned and placed on the bottom chip 105. Thecapillary tool 310 is aligned over the through hole 119 and thereceiving bond pad 127 on the device layer 107 (S420). The capillarytool 310 and bond wire 117 are lowered into the through hole 119 (S425).The melted solder at the end of the bond wire 117 is attached to thereceiver bond pad 127 using compression force and an ultrasonic pulse(S430). The capillary tool 310 is removed from the through hole 119 andthe other end of the bond wire 117 is attached to a corresponding bondpad 115 on the routing layer 111 using compression and an ultrasonicpulse (S435).

While the invention has been shown and described with reference tocertain exemplary embodiments thereof, it will be understood by thoseskilled in the art that various changes in form and details may be madetherein without departing from the spirit and scope of the presentinvention as defined by the appended claims and their equivalents.

The descriptions of the various embodiments of the present inventionhave been presented for purposes of illustration, but are not intendedto be exhaustive or limited to the embodiments disclosed. Manymodifications and variations will be apparent to those of ordinary skillin the art without departing from the scope and spirit of the describedembodiments. The terminology used herein was chosen to best explain theprinciples of the one or more embodiment, the practical application ortechnical improvement over technologies found in the marketplace, or toenable others of ordinary skill in the art to understand the embodimentsdisclosed herein.

1. (canceled)
 2. A quantum computer system comprising: a plurality ofquantum circuits arranged in a two-dimensional layout; and wherein theplurality of quantum circuits includes at least one interior quantumcircuit that is not along a perimeter of the two-dimensional layout,wherein the at least one interior quantum circuit comprises a pluralityof layers, a top layer of the plurality of layers including a throughhole to a bottom layer of the plurality of layers; and a signal wirepositioned at least partially within the through hole and connecting thebottom layer to the top layer.
 3. The quantum computer system of claim2, wherein the bottom layer of the plurality of layers comprises abottom chip having a device layer and the top layer of the plurality oflayers comprises a top chip having a routing layer; and wherein thesignal wire communicatively connects the device layer of the bottom chipto the routing layer of the top chip, and wherein the signal wire is notparallel to a plane of the two dimensional layout.
 4. The quantumcomputer system of claim 3, wherein the through hole is formed byreactive ion etching or by laser milling.
 5. The quantum computer systemof claim 4, wherein the through hole has a diameter less than or equalto 1000 μm.
 6. The quantum computer system of claim 3, wherein theinterior quantum circuit further comprises: a first bonding pad locatedon the device layer; and a second bonding pad located on the routinglayer.
 7. The quantum computer system of claim 6, wherein the signalwire is connected to the first bonding pad and the second bonding pad.8. A quantum computer system comprising: a plurality of quantum circuitsarranged in a two-dimensional layout, the plurality of quantum circuitsincluding at least one interior quantum circuit that is not along aperimeter of the two-dimensional layout, wherein the at least oneinterior quantum circuit includes a device layer and a routing layer; asignal wire that connects the device layer to the routing layer, whereinthe signal wire extends out of the two-dimensional layout of theplurality of quantum circuits; and a through hole formed in the routinglayer, wherein the signal wire pass though the through hole. 9.(canceled)
 10. The quantum computer system of claim 8, wherein thethrough hole is formed by reactive ion etching or by laser milling. 11.The quantum computer system of claim 8, wherein the through hole has adiameter less than or equal to 1000 μm.
 12. The quantum computer systemof claim 8, wherein the interior quantum circuit further comprises: afirst bonding pad located on the device layer; and a second bonding padlocated on the routing layer.
 13. The quantum computer system of claim12, wherein the signal wire is connected to the first bonding pad andthe second bonding pad.
 14. (canceled)